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04-BS-7 · December 2018

Question 4 of 13: Hydraulic Jump — Momentum Force Balance and Flow Rate

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

Reference texts: White, F.M., Fluid Mechanics (8th ed.) — fluid statics and hydrostatic force on plane/curved surfaces incl. gravity-dam stability (Ch. 2), buoyancy and Archimedes' principle (Ch. 2), orifice/nozzle discharge and jet momentum forces (Ch. 3, 6), viscous flow in ducts and the Moody chart (Ch. 6), open-channel flow and the hydraulic jump (Ch. 10), drag and stability of bluff bodies (Ch. 7), turbomachinery and jet propulsion (Ch. 11).

Question 4: Hydraulic Jump — Momentum Force Balance and Flow Rate (5 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given.

QuantityValue
Channel width, $b$2.4 m
Depth before jump, $y_1$0.4 m
Depth after jump, $y_2$2.6 m
y1=0.4 m, V1 (fast, shallow) y2=2.6 m, V2 (slow, deep) jump
Hydraulic jump: supercritical inflow (shallow, fast) transitions abruptly to subcritical outflow (deep, slow).

Find. (a) The momentum force balance across the jump in terms of $V_1,V_2$; (b) the volume flow rate $Q$.

Approach. Apply the momentum equation to a control volume spanning the jump: the net hydrostatic pressure force difference between the two sections equals the rate of change of momentum flux. Combined with continuity ($Q=by_1V_1=by_2V_2$), this gives two equations in the two unknowns $V_1,V_2$ (equivalently, one equation in $Q$).

  1. Part (a) — momentum force balance. The hydrostatic thrust at each section is $F_i=\tfrac12\rho g y_i^2 b$; the momentum equation for the control volume between sections 1 and 2 is $$F_1-F_2=\dot{m}(V_2-V_1)=\rho Q(V_2-V_1)$$ $$\boxed{\tfrac12\rho g b\left(y_1^2-y_2^2\right)=\rho Q\left(V_2-V_1\right)}$$ — the net hydrostatic push from the shallow side exceeds that from the deep side, and this net force is exactly what decelerates the flow from $V_1$ to the much smaller $V_2$.
  2. Part (b) — eliminate $V_1,V_2$ using continuity. From continuity $V_1=Q/(by_1)$, $V_2=Q/(by_2)$; substituting into the momentum balance and solving for $Q$, $$Q^2=\frac{\tfrac12gb^2\left(y_1^2-y_2^2\right)}{\left(1/y_2-1/y_1\right)}=\frac{\tfrac12(9.81)(2.4)^2\left(0.4^2-2.6^2\right)}{\left(1/2.6-1/0.4\right)}$$ $$Q=\boxed{9.39\ \text{m}^3/\text{s}}$$
  3. Resulting velocities (for the force-balance check and for Question 5). $$V_1=\frac{Q}{by_1}=\frac{9.39}{(2.4)(0.4)}=\boxed{9.78\ \text{m/s}}\qquad V_2=\frac{Q}{by_2}=\frac{9.39}{(2.4)(2.6)}=\boxed{1.505\ \text{m/s}}$$ The upstream Froude number $Fr_1=V_1/\sqrt{gy_1}=9.78/\sqrt{(9.81)(0.4)}=4.94\gt1$ confirms the upstream flow is indeed supercritical, consistent with a jump forming.
QuantityValue
Momentum force balance$\tfrac12\rho g b(y_1^2-y_2^2)=\rho Q(V_2-V_1)$
Flow rate, Q9.39 m³/s
V1 / V29.78 / 1.505 m/s
Upstream Froude number, Fr14.94 (supercritical)
Check: this derived Q = 9.39 m³/s agrees to within 0.1% with the 9.4 m³/s flow rate GIVEN directly in Question 5 for the same channel and depths — a strong internal cross-check that the momentum-and-continuity solution here is correct.